Motion in Polyethylene. II. Vibrations in Crystalline Polyethylene

Abstract
Using the specific heats of completely crystalline polyethylene as a basis, the vibrational spectrum is discussed. The vibrational spectrum is found to consist of three completely separate parts. (A) The high‐frequency CH2‐stretching vibrations between 2850 and 2930 cm—1 which contribute little to the specific heat below 350°K. (B) The low‐frequency optical vibrations between 720 and 1480 cm—1 which contribute above 150°K increasingly to the specific heat. (C) The acoustical vibrations which stretch from zero to approximately 500 cm—1 and are at 260°K to 90% excited. A and B are adequately known from infrared and Raman experiments. C can be approximated by a Tarasov‐type treatment leading to θ temperatures of 123° and 540° for the three‐dimensional and one‐dimensional parts, respectively. More detailed spectra are discussed, and a semiempirical best fit is given. The one‐dimensional Debye function necessary for this discussion has been computed to five places and is tabulated in steps of hν/kT=0.01.

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